Category: PARP

We assume that the angular displacement,a(t), is superposed by additive distributed white sound with no mean and variance2 normally, denoted bye(t): In this full case, the variance from the Fourier coefficient from the angular displacement on the sampling period of lengthLis distributed by We calculate the proper period program,e(t), from the sound by subtracting the harmonic oscillation,a(t), distributed by the Fourier coefficients (fa) and (fa) from the initial measurement

We assume that the angular displacement,a(t), is superposed by additive distributed white sound with no mean and variance2 normally, denoted bye(t): In this full case, […]

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